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通过应力诱导磁各向异性实现富铁非晶微丝的磁软特性及畴壁动力学调控

Engineering of Magnetic Softness and Domain Wall Dynamics of Fe-rich Amorphous Microwires by Stress- induced Magnetic Anisotropy.

作者信息

Corte-León P, Blanco J M, Zhukova V, Ipatov M, Gonzalez J, Churyukanova M, Taskaev S, Zhukov A

机构信息

Dpto. Física de Materiales, Fac. Químicas, UPV/EHU, 20018, San Sebastian, Spain.

Dpto. de Física Aplicada, EIG, UPV/EHU, 20018, San Sebastian, Spain.

出版信息

Sci Rep. 2019 Aug 27;9(1):12427. doi: 10.1038/s41598-019-48755-4.

DOI:10.1038/s41598-019-48755-4
PMID:31455829
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6711959/
Abstract

We observed a remarkable improvement of domain wall (DW) mobility, DW velocity, giant magnetoimpedance (GMI) effect and magnetic softening at appropriate stress-annealing conditions. Beneficial effect of stress-annealing on GMI effect and DW dynamics is associated with the induced transverse magnetic anisotropy. An improvement of the circumferential permeability in the nearly surface area of metallic nucleus is evidenced from observed magnetic softening and remarkable GMI effect rising. We assumed that the outer domain shell with transverse magnetic anisotropy associated to stress-annealing induced transverse magnetic anisotropy affects the travelling DW in a similar way as application of transversal bias magnetic field allowing enhancement the DW velocity. Observed decreasing of the half-width of the EMF peak in stress-annealed microwires can be associated to the decreasing of the characteristic DW width. Consequently, stress annealing enabled us to design the magnetic anisotropy distribution beneficial for optimization of either GMI effect or DW dynamics.

摘要

我们观察到,在适当的应力退火条件下,畴壁(DW)迁移率、DW速度、巨磁阻抗(GMI)效应和磁软化有显著改善。应力退火对GMI效应和DW动力学的有益影响与诱导的横向磁各向异性有关。从观察到的磁软化和显著的GMI效应增强可以证明,金属核近表面区域的圆周磁导率有所提高。我们假设,与应力退火诱导的横向磁各向异性相关的具有横向磁各向异性的外畴壳,以与施加横向偏置磁场类似的方式影响移动的DW,从而提高DW速度。在应力退火微丝中观察到的EMF峰值半高宽的减小可能与特征DW宽度的减小有关。因此,应力退火使我们能够设计出有利于优化GMI效应或DW动力学的磁各向异性分布。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/cea8a4db4e0e/41598_2019_48755_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/d57934ab5ca6/41598_2019_48755_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/f862aa205c40/41598_2019_48755_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/7272389d3318/41598_2019_48755_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/724d8f954b59/41598_2019_48755_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/dfe257e62c82/41598_2019_48755_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/ab8243c972c0/41598_2019_48755_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/503b162d8fc9/41598_2019_48755_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/e980ed54308e/41598_2019_48755_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/cea8a4db4e0e/41598_2019_48755_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/d57934ab5ca6/41598_2019_48755_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/f862aa205c40/41598_2019_48755_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/7272389d3318/41598_2019_48755_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/724d8f954b59/41598_2019_48755_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/dfe257e62c82/41598_2019_48755_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/ab8243c972c0/41598_2019_48755_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/503b162d8fc9/41598_2019_48755_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/e980ed54308e/41598_2019_48755_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1234/6711959/cea8a4db4e0e/41598_2019_48755_Fig9_HTML.jpg

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